Chiral superconducting trial wavefunctions (Pfaffian and K2a) have lower variational energy than an optimized quarter Fermi liquid in a rhombohedral graphene model near the flat-band regime.
Pairing via Index theorem
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abstract
This work is motivated by a specific point of view: at short distances and high energies the undoped and underdoped cuprates resemble the $\pi$-flux phase of the t-J model. The purpose of this paper is to present a mechanism by which pairing grows out of the doped $\pi$-flux phase. According to this mechanism pairing symmetry is determined by a parameter controlling the quantum tunneling of gauge flux quanta. For zero tunneling the symmetry is $d_{x^2-y^2}+id_{xy}$, while for large tunneling it is $d_{x^2-y^2}$. A zero-temperature critical point separates these two limits.
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Variational Monte Carlo Optimization of Topological Chiral Superconductors
Chiral superconducting trial wavefunctions (Pfaffian and K2a) have lower variational energy than an optimized quarter Fermi liquid in a rhombohedral graphene model near the flat-band regime.